Search results for "VIOLATION"

showing 10 items of 540 documents

CP Violation in Correlated Production and Decay of Unstable Particles

2011

We study resonant CP-violating Einstein--Podolsky--Rosen correlations that may take place in the production and decay of unstable scalar particles at high-energy colliders. We show that as a consequence of unitarity and CPT invariance of the S-matrix, in 2 --> 2 scatterings mediated by mixed scalar particles, at least three linearly independent decay matrices associated with the unstable scalar states are needed to obtain non-zero CP-odd observables that are also odd under C-conjugation. Instead, for the correlated production and decay of two unstable particle systems in 2 --> 4 processes, we find that only two independent decay matrices are sufficient to induce a net non-vanishing CP…

Particle systemPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityBranching fractionCPT symmetryScalar (mathematics)FOS: Physical sciencesObservableHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelParticle Physics - Phenomenology
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First observation of the doubly charmed baryon decay Ξcc++→Ξc+π+

2018

The doubly charmed baryon decay Ξcc++→Ξc+π+ is observed for the first time, with a statistical significance of 5.9σ, confirming a recent observation of the baryon in the Λc+K−π+π+ final state. The data sample used corresponds to an integrated luminosity of 1.7 fb−1, collected by the LHCb experiment in pp collisions at a center-of-mass energy of 13 TeV. The Ξcc++ mass is measured to be 3620.6±1.5(stat)±0.4(syst)±0.3(Ξc+) MeV/c2 and is consistent with the previous result. The ratio of branching fractions between the decay modes is measured to be [B(Ξcc++→Ξc+π+)×B(Ξc+→pK−π+)]/[B(Ξcc++→Λc+K−π+π+)×B(Λc+→pK−π+)]=0.035±0.009(stat)±0.003(syst).

Particles and fieldGeneral Physics and Astronomy01 natural sciencesNONuclear physicsPhysics and Astronomy (all)Condensed Matter::Superconductivity0103 physical sciencesPhysicLHCb - Abteilung HintonSDG 7 - Affordable and Clean Energy010306 general physicsPhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energy010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyParticle physicsHEPBaryonLHCbCharmed baryonHadron colliderHigh Energy Physics::ExperimentB physics Branching fraction CP violation Hadron-Hadron scattering (experiments)LHCFísica de partículesExperiments
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Superbeams plus neutrino factory: The golden path to leptonic CP violation

2002

Superbeams (SB) and Neutrino Factories (NF) are not alternative facilities for exploring neutrino oscillation physics, but successive steps. The correct strategy is to contemplate the combination of their expected physics results. We show its important potential on the disappearance of fake degenerate solutions in the simultaneous measurement of $\theta_{13}$ and leptonic CP violation. Intrinsic, sign($\Delta m_{13}^2$) and $\theta_{23}$ degeneracies are shown to be extensively eliminated when the results from one NF baseline and a SB facility are combined. A key point is the different average neutrino energy and baseline of the facilities. For values of $\theta_{13}$ near its present limit…

Path (topology)PhysicsNuclear and High Energy PhysicsParticle physicsDegenerate energy levelsFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)CP violationFísica nuclearNeutrino FactoryNeutrinoNeutrino oscillationEnergy (signal processing)Particle Physics - PhenomenologySign (mathematics)
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Measurement of the D→K−π+ strong phase difference in ψ(3770)→D0D¯0

2014

Abstract We study D 0 D ¯ 0 pairs produced in e + e − collisions at s = 3.773 GeV using a data sample of 2.92 fb−1 collected with the BESIII detector. We measured the asymmetry A K π CP of the branching fractions of D → K − π + in CP-odd and CP-even eigenstates to be ( 12.7 ± 1.3 ± 0.7 ) × 10 − 2 . A K π CP can be used to extract the strong phase difference δ K π between the doubly Cabibbo-suppressed process D ¯ 0 → K − π + and the Cabibbo-favored process D 0 → K − π + . Using world-average values of external parameters, we obtain cos δ K π = 1.02 ± 0.11 ± 0.06 ± 0.01 . Here, the first and second uncertainties are statistical and systematic, respectively, while the third uncertainty arises …

Phase differencePhysicsNuclear and High Energy Physicsmedia_common.quotation_subjectElectron–positron annihilationQuantum mechanicsAnalytical chemistryPiCP violation7. Clean energyAsymmetrymedia_commonPhysics Letters B
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A measurement of the phases of the CP-violating amplitudes in K0→2π decays and a test of CPT invariance

1990

Abstract The phases of the CP-violating amplitudes in K0→π+π− and K0→2π0 decays, φ+−=46.9°±2.2° and φ00=47.1°±2.8°, have been measured in the same experiment, and a direct comparison gives the phase difference φ00−φ+−=0.2°±2.9°. This result leads to an upper limit on possible CPT violation in the K0 mass matrix, of |(m K 0 −m K 0 )/m K 0 | −18 at the 95% confidence level and is the most stringent test of the equality of particle and antiparticle masses.

Phase differencePhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsAntiparticleAmplitudeCPT symmetryCP violationLimit (mathematics)Mass matrixlcsh:Physicslcsh:QC1-999Physics Letters B
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Roadmap on STIRAP applications

2019

STIRAP (stimulated Raman adiabatic passage) is a powerful laser-based method, usually involving two photons, for efficient and selective transfer of populations between quantum states. A particularly interesting feature is the fact that the coupling between the initial and the final quantum states is via an intermediate state, even though the lifetime of the latter can be much shorter than the interaction time with the laser radiation. Nevertheless, spontaneous emission from the intermediate state is prevented by quantum interference. Maintaining the coherence between the initial and final state throughout the transfer process is crucial. STIRAP was initially developed with applications in …

PhotonAtomic Physics (physics.atom-ph)Digital storageStimulated Raman adiabatic passage02 engineering and technologyStimulated Raman adiabatic passage (STIRAP)01 natural scienceslaw.inventionPhysics - Atomic PhysicsFTIR SPECTROSCOPYstimulated Raman adiabatic passage (STIRAP)lawStereochemistryRare earthsStatistical physicsMetal ionsmolecular Rydberg statesQCparity violationPhysicseducation.field_of_studyQuantum PhysicsElectric dipole momentsCoherent population transfer021001 nanoscience & nanotechnologyCondensed Matter Physicsacoustic waves; molecular Rydberg states; nuclear coherent population transfer; parity violation; spin waves; stimulated Raman adiabatic passage (STIRAP); ultracold moleculesADIABATIC PASSAGEAtomic and Molecular Physics and OpticsChemical DynamicsMolecular beamsVIOLATING ENERGY DIFFERENCEResearch group A. Pálffy – Division C. H. KeitelStimulated emission0210 nano-technologyCoherence (physics)Experimental parametersPopulationFOS: Physical sciencesacoustic waves530spin wavesMolecular Rydberg statesELECTROMAGNETICALLY INDUCED TRANSPARENCYSINGLE PHOTONSQuantum statePhysics - Chemical Physics0103 physical sciencesUltracold moleculesSpontaneous emissionddc:530Nuclear coherent population transfer010306 general physicseducationStimulated Raman adiabatic passageChemical Physics (physics.chem-ph)Rare-earth-ion doped crystalsPhotonsQuantum opticsnuclear coherent population transferBROAD-BANDControlled manipulationsPOLAR-MOLECULESMoleculesRydberg statesLaserSuperconducting quantum circuitAcoustic wavesParity violationstimulated Raman adiabatic passage (STIRAP); ultracold molecules; parity violation; spin waves; acoustic waves; molecular Rydberg states; nuclear coherent population transferDewey Decimal Classification::500 | Naturwissenschaften::530 | Physikultracold moleculesQuantum Physics (quant-ph)QUANTUM GASSpin waves
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Measurement of the permanent electric dipole moment of the neutron

2020

We present the result of an experiment to measure the electric dipole moment (EDM) of the neutron at the Paul Scherrer Institute using Ramsey’s method of separated oscillating magnetic fields with ultracold neutrons. Our measurement stands in the long history of EDM experiments probing physics violating time-reversal invariance. The salient features of this experiment were the use of a 199Hg comagnetometer and an array of optically pumped cesium vapor magnetometers to cancel and correct for magnetic-field changes. The statistical analysis was performed on blinded datasets by two separate groups, while the estimation of systematic effects profited from an unprecedented knowledge of the magne…

Physics - Instrumentation and DetectorsMagnetometerFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesMeasure (mathematics)S017EDMlaw.inventionHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)statistical analysislawcesium0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]time reversal: invarianceStatistical analysisNeutronNuclear Physics - ExperimentPhysics::Atomic Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)Detectors and Experimental Techniques010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsn: electric momentInstrumentation and Detectors (physics.ins-det)Cesium vaporMagnetic fieldElectric dipole moment* Automatic Keywords *Ultracold neutronsElementary Particles and FieldshistoryAtomic physicstime reversal: violationmagnetic field: oscillationParticle Physics - Experiment
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Comparison of ultracold neutron sources for fundamental physics measurements

2016

Ultracold neutrons (UCNs) are key for precision studies of fundamental parameters of the neutron and in searches for new CP violating processes or exotic interactions beyond the Standard Model of particle physics. The most prominent example is the search for a permanent electric dipole moment of the neutron (nEDM). We have performed an experimental comparison of the leading UCN sources currently operating. We have used a 'standard' UCN storage bottle with a volume of 32 liters, comparable in size to nEDM experiments, which allows us to compare the UCN density available at a given beam port.

Physics - Instrumentation and DetectorsPhysics beyond the Standard ModelFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physics25.40Fq0103 physical sciencesCP: violationNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear ExperimentPhysicsn: densityn: electric moment010308 nuclear & particles physics29.25.Dzn: particle sourceInstrumentation and Detectors (physics.ins-det)31.30.jn28.20.Pr3. Good healthFundamental physicsMoment (physics)14.20.DhUltracold neutronsNeutron sourceBeam (structure)
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The MORA project

2018

The MORA (Matter's Origin from the RadioActivity of trapped and oriented ions) project aims at measuring with unprecedented precision the D correlation in the nuclear beta decay of trapped and oriented ions. The D correlation offers the possibility to search for new CP-violating interactions, complementary to searches done at the LHC and with Electric Dipole Moments. Technically, MORA uses an innovative in-trap orientation method which combines the high trapping efficiency of a transparent Paul trap with laser orientation techniques. The trapping, detection, and laser setups are under development, for first tests at the Accelerator laboratory, JYFL, in the coming years.

Physics - Instrumentation and Detectorsexperimental methodsPhysics beyond the Standard Model42.25.Janucl-ex01 natural sciences7. Clean energylaw.invention23.40.-slawPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Detectors and Experimental TechniquesNuclear Experimentphysics.ins-detPhysicsLarge Hadron Colliderion trapsOrientation (computer vision)Instrumentation and Detectors (physics.ins-det)Condensed Matter PhysicsComputer Science::Computers and SocietyAtomic and Molecular Physics and OpticsIon trapydinfysiikkaNuclear and High Energy PhysicsFOS: Physical sciencesTrapping[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Computer Science::Digital LibrariesIonFundamental symmetriesNuclear physics0103 physical sciencesCP: violation37.10.TyNuclear Physics - Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Physical and Theoretical Chemistry010306 general physicsactivity reportion: capturenucleus: semileptonic decayCondensed Matter::Quantum Gases010308 nuclear & particles physicsBeta DecayLaserlaserDipoleefficiencycorrelationfundamental symmetries11.30.Erbeta decayIon traps
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Search for heavy neutrinos and right-handed W bosons in events with two leptons and jets in pp collisions at √s=7 TeV with the ATLAS detector

2012

This letter reports on a search for hypothetical heavy neutrinos, N, and right-handed gauge bosons, WR, in events with high transverse momentum objects which include two reconstructed leptons and at least one hadronic jet. The results were obtained from data corresponding to an integrated luminosity of 2.1 fb−1 collected in proton–proton collisions at √s=7 TeV with the ATLAS detector at the CERN Large Hadron Collider. No excess above the Standard Model background expectation is observed. Excluded mass regions for Majorana and Dirac neutrinos are presented using two approaches for interactions that violate lepton and lepton-flavor numbers. One approach uses an effective operator framework, t…

Physics and Astronomy (miscellaneous)Atlas detector01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]w bosonNuclear ExperimentDetectors de radiacióBosonMajorana Neutrinosddc:539PhysicsRight handedSettore FIS/01 - Fisica SperimentaleHadron-Hadron Scattering; ATLAS detectorATLASParityPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNeutrinoParticle Physics - ExperimentParticle physicsOscillationsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasLEFT-RIGHT SYMMETRYGauge bosonScience & TechnologyATLAS detectorViolation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaParity (physics)LepMassEnergiesPair productionCol·lisions (Física nuclear)Experimental High Energy Physicsproton-proton collisionsHigh Energy Physics::ExperimentLepton
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